EE130/230M Review Session 1.Small Signal Models for MOSFET/BJT 2.MOS Electrostatics.
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Transcript of EE130/230M Review Session 1.Small Signal Models for MOSFET/BJT 2.MOS Electrostatics.
EE130/230M Review Session
1. Small Signal Models for MOSFET/BJT
2. MOS Electrostatics
BJT Small Signal Model
• A small change in IB or VBE will result in a small change in IC and VCE
• input current = be( 1 / )j C r v
output current = m beg v
the cutoff frequency (wT = 2pfT) is defined at
• input voltage = bev
output voltage =
= d1 / dg i
be/m dg g vvbe
r gmvbe
C
E
B
E
C
+
,
,
( )1 / /
1 1
1 / /
c m m
b m dc F m J BE
dc F J BE C
i g g
i r j C g j g C
j C kT qI
Example
A BJT is biased at IC = 1 mA and VCE = 3V. bdc = 90, tF = 5ps, T = 300K. Find (a) gm , (b) rp , (c) Cp .
Solution:
(a)
(b) rp = bdc / gm = 90/0.039 = 2.3 kW
(c)
siemens)(milliqkTIg Cm mS 39V
mA39
mV 26
mA 1)//(
ad)(femto fargC mF fF 19F109.1039.0105 1412
EE130/230M Spring 2013 Lecture 27, Slide 3
MOSFET Small Signal Model
• A small change in VG will result in a small change in ID and VDS
• input current = g gj C v
output current = m gg v
m g
T g g
12
g v
f C v
the cutoff frequency (wT = 2pfT) is defined at
• input voltage = gv
output voltage =
= d1 / dg i
g/m dg g v
Summary of Small Signal Models
• Inputs/Outputs
• Linearized equivalent circuits
• Key components
• Performances Gain Cut-off frequency
MOS Capacitor Energy Band Diagram
Since the substrate is n-type, this is a PMOS capacitor, i.e. a sufficiently large negative gate voltage is required to deplete the semiconductor surface of mobile electrons and form an inversion-layer of holes there.
a) Assuming that the n-type Si substrate is non-degenerately doped, its work function is
S = χ + (EC-EF) = χ + EG/2 – (kT/q)∙ln(ND/ni) = 4.05 eV + 0.56 eV – 0.48 eV = 4.13 eV
The gate material is heavily doped p-type silicon with work function χ + EG 5.2 eV
Ideally, the flat-band voltage is given by the difference between the gate and the semiconductor work functions:
qVFB= M – S 5.2 eV – 4.13 eV = 1.07 eV
Therefore the flat-band voltage VFB 1.07 V
Consider an ideal MOS capacitor maintained at T = 300K with the following parameters: • Gate material is p+ polycrystalline-silicon (work function M = 5.2 eV) • Substrate is n-type Si, with doping concentration 1018 cm-3 (assume that this is non-
degenerate) • Oxide thickness xo = 2 nm
a) What is the flat-band voltage, VFB, of this capacitor? b) Sketch the energy-band diagrams, labeling qVG, qS, qVox (no numerical values required), for the
following bias conditions: i) flat band ii) accumulation iii) equilibrium iv) strong inversion
Problem:
Solution:
Flat-band Conditiona) The band diagrams corresponding to the various regions of operation are drawn below:
i) Flat-band condition: VG = VFB so that there is no band-bending
Equilibrium Conditioni) Equilibrium: Metal and Si Fermi levels are equal, VG = 0 V
Note that the surface is depleted of mobile electrons, i.e. there is a depletion region (of width W) at the surface of the Si.
Accumulation Conditioni) Accumulation: VG > VFB so that there are majority carrier electrons accumulated at the Si surface
Strong Inversion Conditioni) Strong inversion: VG is more negative than the threshold voltage VT, so that the surface is strongly p-type,
i.e. with a (mobile) hole density greater than the (immobile) density of ionized donor atoms. The depletion region has a width WT, and the total voltage dropped across the Si F = 2F = -2(kT/q)∙ln(ND/ni)=-0.96 V.
Charge distribution
Charge amount
Capacitance
Equivalent circuits
MOS Capacitor Charge vs. Gate Voltage
Accumulation Depletion Inversion
VT
Flat-band voltageMaximum depletion charge
C (pF)
Vg (V)
70
0.25 -0.7
MOS Capacitance vs. Gate Voltage
Accumulation
DepletionInversion
VTFlat-band voltage
Minimum capacitance